Range of researches in theoretical physics

Interests and results are presented

Dr. A. Mazurenko


       Obtaining of the exact analytical solutions for steady-state Schrodinger equations ( C0 º - h2 /(8 p2 m) is constant)

æ
ç
è
C0  d2
d x2
  +  U(x) ö
÷
ø
  Y(x)   =   E  Y(x)
(1)
on a plane
æ
ç
è
C0  d2
d x2
  +  C0  d2
d y2
  +  U(x,y) ö
÷
ø
  Y(x,y)   =   E  Y(x,y)
(2)
in space
( C0 D  +  U(r))   Y(r)   =   E  Y(r)
(3)
for new special cases of potential functions U(r) . The function U(r) depends on both module and direction of the multidimensional vector r .

       To solve the equations the author specially constructed functions fn (z) which are orthogonal on a contour L


ó
õ
L 
fn (z) fm (z)  dM(z)   =   dm, n  dn2
(4)
with a measure M(z) .

       Functions generalizing orthogonal polynomials of the Jacobi Pn(a,  b) (x) of continuous argument x are determined.

       The polynomials pn (x,b) ( fn (z) º pn (z,b) ) which are orthogonal on interval [-1,  1] (the contour L is non-closed and coincides with interval [-1,  1] ) with respect to different weight functions s(x,b) ( M(z)   =   ò0z  s(x,b)  dx    +  C ) have been constructed.

Name of constructed polynomials pn (x,b) Weight s(x,b) in orthogonality relation
Christoffel-Legendre-1
s(x,b)   =    (b-x)
b
  ,    b ³ 1
Christoffel-Jacobi-1
s(x,b)   =    (b-x)
b
  (1-x)a(1+x)b,    b ³ 1,    a > -1,    b > -1
Uvarov-Legendre-1
s(x,b)   =    b
(b-x)
  ,    b ³ 1
Christoffel-Legendre-2
s(x,b)   =    (b2-x2)
b2
  ,    b ³ 1
Uvarov-Legendre-2
s(x,b)   =    b2
(b2-x2)
  ,   b ³ 1
Christoffel-Legendre-4
s(x,b)   =    (b12 -x2) (b22 -x2 )
(b1  b2 )2
  ,    ì
í
î
b1 ³ 1 and b2 ³ 1       
"b Î Re     b = b1 º b2

       Christoffel-Krawtchouk and nonclassical Gegenbauer polynomials fn (z = m) º pn (m) with discrete weights s(m) have been constructed. The orthogonality relation for polynomials of a discrete variable has a stepwise measure

M(z)   =    z
ó
õ
-¥ 

å
<
m 
s(m)  d(x-m)  dx    +  C   º   
å
<
m 
s(m)  q(x-m)    +  C
(5)
where d(z) º [d/d z] q(z) is the Dirac delta-function and q(z) is the Heaviside function
q(z)   º    ì
í
î
1 ,    if  z ³ 0 ;
0 ,    if  z < 0 .
(6)

Latex source file:  theorph.zip 1,5 kb.


File translated from TEX by TTH, version 2.57.

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